Imaging lens

ABSTRACT

A compact low-profile low-cost imaging lens with a small F-value which offers a wide field of view and corrects aberrations properly. Its elements are spaced from each other and arranged from an object side to an image side as follows: a first positive lens having a convex object-side surface; a second negative lens; a third positive or negative lens; a fourth positive or negative lens; a fifth positive or negative lens; a sixth positive or negative lens; and a seventh lens as a double-sided aspheric lens having a concave image-side surface. The third to sixth lenses each have at least one aspheric surface. The aspheric image-side surface of the seventh lens has a pole-change point off an optical axis. The imaging lens satisfies a conditional expression −1.0&lt;f1/f2&lt;−0.15, where f1 denotes focal length of the first lens, and f2 denotes focal length of the second lens.

The present application is based on and claims priority of Japanesepatent application No. 2014-220092 filed on Oct. 29, 2014, the entirecontents of which are hereby incorporated by reference.

BACKGROUND OF THE INVENTION Field of the Invention

The present invention relates to an imaging lens which forms an image ofan object on a solid-state image sensor such as a CCD sensor or a C-MOSsensor used in a compact image pickup device, and more particularly toan imaging lens which is built in an image pickup device mounted in anincreasingly compact and low-profile mobile terminal such as asmartphone, mobile phone, tablet or PDA (Personal Digital Assistant), ora game console, or an information terminal such as a PC, or a highlyfunctional product such as a home appliance with a camera function.

Description of the Related Art

In recent years, there has been a general tendency that many informationterminals have a camera function. Also, home appliances with a cameraare becoming widely used. For example, by telecommunication between ahome appliance and a smartphone, a user away from home can monitor inreal time what is going on at home or check how his/her child or pet isat home or control the home appliance to optimize its operation.Furthermore, wearable devices, such as glasses with a camera functionand wrist watches with a camera function, have appeared in the market.It is thought that a variety of high value-added products which enhanceconsumer convenience and consumer satisfaction will be increasinglydeveloped in the future by adding a camera function to various existingproducts. The cameras mounted in such products are required not only toprovide high resolution to cope with an increase in the number of pixelsbut also to be compact and low-profile and offer high brightness and awide field of view.

However, in order to provide a low-profile imaging lens with highbrightness and a wide field of view as described above, the problem withdifficulty in correction of aberrations in the peripheral area of animage has to be addressed, and unless the problem is solved, it will bedifficult to deliver high imaging performance throughout the image.

With the recent trend toward image sensors which deal with an increasingnumber of pixels, an imaging lens composed of seven constituent lensesis expected to properly correct such aberrations in the peripheral areaof an image that cannot be corrected properly by an imaging lenscomposed of six constituent lenses and also thought to have potential tocorrect various aberrations properly and achieve compactness, a smallF-value and a wide field of view in a balanced manner. For example, theimaging lens described in JP-A-2012-155223 (Patent Document 1) is knownas such an imaging lens composed of seven constituent lenses.

Patent Document 1 discloses an imaging lens which includes, in orderfrom an object side, a first biconvex lens, a second biconcave lenscemented with the first lens, a third negative meniscus lens having aconvex surface on the object side, a fourth positive meniscus lenshaving a concave surface on the object side, a fifth negative meniscuslens having a convex surface on the object side, a sixth biconvex lens,and a seventh biconcave lens. In this imaging lens, the ratio betweenthe focal length of the front lens group composed of the first to fourthlenses and the focal length of the back lens group composed of the fifthto seventh lenses is kept within a prescribed range so that the opticalsystem is compact and various aberrations are corrected properly.

The imaging lens composed of seven constituent lenses as described inPatent Document 1 corrects various aberrations properly and offersrelatively high brightness with an F-value from 2.09 to 2.35 and arelatively wide field of view of 33 degrees. However, the total tracklength is longer than the diagonal length of the effective imaging planeof the image sensor, so that it is difficult to apply the imaging lensto a device which is strongly expected to be compact and low-profile. Ifthis lens system is designed to offer a wider field of view and higherbrightness, it would be unable to correct aberrations in the peripheralarea properly. Consequently, it would be difficult to reduce imageartifacts throughout the image effectively and ensure high imagequality. Furthermore, the manufacture of a cemented lens requires highprecision manufacturing techniques because it involves troublesomealignment and lamination steps, so that it is difficult to mass-producethe imaging lens at low cost with high productivity.

As mentioned above, in the conventional art, it is difficult to providea low-profile low-cost imaging lens which offers high brightness, highresolution and a wide field of view.

SUMMARY OF THE INVENTION

The present invention has been made in view of the above problem, and anobject thereof is to provide a compact low-cost imaging lens which meetsthe demand for low-profileness, offers high brightness and a wide fieldof view and corrects various aberrations properly.

Here, “low-profile” implies that total track length is shorter than thediagonal length of the effective imaging plane of the image sensor and“wide field of view” implies that the field of view is 70 degrees ormore. The diagonal length of the effective imaging plane of the imagesensor is considered equal to the diameter of an effective image circlewhose radius is the maximum image height, that is, the vertical heightfrom an optical axis to the point where a light ray incident on theimaging lens at a maximum field of view enters the image plane.

In the present invention, a convex surface or a concave surface meansthat the paraxial portion of the surface (portion near the optical axis)is convex or concave. A “pole-change point” on an aspheric surface meansa point on the aspheric surface at which a tangential plane intersectsthe optical axis perpendicularly. The values of total track length andback focus are defined to express distances on the optical axis in whichan optical element such as an IR cut filter or cover glass is removed.

In order to address the above problem, according to an aspect of thepresent invention, there is provided an imaging lens composed of sevenconstituent lenses which forms an image of an object on a solid-stateimage sensor, in which the lenses are arranged in order from an objectside to an image side as follows:

a first lens with positive refractive power having a convex surface onthe object side; a second lens with negative refractive power; a thirdlens with positive or negative refractive power; a fourth lens withpositive or negative refractive power; a fifth lens with positive ornegative refractive power; a sixth lens with positive or negativerefractive power; and a seventh lens as a double-sided aspheric lenshaving a concave surface on the image side. These constituent lenses arespaced from each other. The third to sixth lenses each have at least oneaspheric surface, and the seventh lens has pole-change points off anoptical axis on the aspheric image-side surface. The imaging lenssatisfies a conditional expression (1) below:

−1.0<f1/f2<−0.15   (1)

where f1 denotes the focal length of the first lens, and f2 denotes thefocal length of the second lens.

In the imaging lens composed of seven constituent lenses, the first lenshas strong refractive power to achieve low-profileness and the secondlens corrects spherical aberrations and chromatic aberrations properly.The third lens, the fourth lens, the fifth lens, and the sixth lens eachhave at least one aspheric surface and are given appropriated positiveor negative refractive power to ensure low-profileness and a wide fieldof view and correct off-axial aberrations such as astigmatism, fieldcurvature and distortion. The seventh lens, a lens with positive ornegative refractive power having a concave surface on the image side,corrects spherical aberrations and field curvature and distortion in theperipheral area using its aspheric surfaces. Also, since the image-sidesurface of the seventh lens has an aspheric shape with pole-changepoints, the angle of rays incident on the image sensor is controlledappropriately.

In the present invention, no cemented lens is used and all theconstituent lenses are spaced from each other so that the number ofaspheric surfaces can be increased to correct aberrations properly anddeliver higher performance.

The conditional expression (1) defines an appropriate range for theratio of the focal length of the first lens to the focal length of thesecond lens, and indicates a condition to achieve low-profileness andcorrect chromatic aberrations properly. If the value is above the upperlimit of the conditional expression (1), the refractive power of thefirst lens would be too strong for the second lens to properly correctchromatic aberrations which occur on the first lens, though it would beadvantageous in shortening the total track length. On the other hand, ifthe value is below the lower limit of the conditional expression (1),the refractive power of the first lens would be too weak to shorten thetotal track length.

If the fifth lens has positive refractive power and the sixth lens hasnegative refractive power, preferably the imaging lens according to thepresent invention satisfies a conditional expression (2) below:

0.5<f5/f<1.5   (2)

where

-   -   f: focal length of the overall optical system of the imaging        lens, and    -   f5: focal length of the fifth lens.

The conditional expression (2) defines an appropriate range for theratio of the focal length of the fifth lens to the focal length of theoverall optical system of the imaging lens, and indicates a condition toachieve low-profileness and correct spherical aberrations and comaaberrations properly, provided that the fifth lens has positiverefractive power and the sixth lens has negative refractive power. Ifthe value is above the upper limit of the conditional expression (2),the refractive power of the fifth lens would be too weak to shorten thetotal track length. On the other hand, if the value is below the lowerlimit of the conditional expression (2), the refractive power of thefifth lens would be too strong and spherical aberrations and comaaberrations would increase, thereby making it difficult to correctaberrations, though it would be advantageous in shortening the totaltrack length.

If the fifth lens has positive refractive power and the sixth lens hasnegative refractive power, preferably the imaging lens according to thepresent invention satisfies a conditional expression (3) below:

−8.0<f6/f<−1.0   (3)

where

-   -   f: focal length of the overall optical system of the imaging        lens, and    -   f6: focal length of the sixth lens.

The conditional expression (3) defines an appropriate range for theratio of the focal length of the sixth lens to the focal length of theoverall optical system of the imaging lens, and indicates a condition toachieve low-profileness and correct chromatic aberrations properly,provided that the fifth lens has positive refractive power and the sixthlens has negative refractive power. If the value is above the upperlimit of the conditional expression (3), the negative refractive powerof the sixth lens would be too strong to shorten the total track length.On the other hand, if the value is below the lower limit of theconditional expression (3), the negative refractive power of the sixthlens would be too weak to correct chromatic aberrations properly.

If the fifth lens has negative refractive power and the sixth lens haspositive refractive power, preferably the imaging lens according to thepresent invention satisfies a conditional expression (4) below:

−20<f5/f<−1.0   (4)

where

-   -   f: focal length of the overall optical system of the imaging        lens, and    -   f5: focal length of the fifth lens.

The conditional expression (4) defines an appropriate range for theratio of the focal length of the fifth lens to the focal length of theoverall optical system of the imaging lens, and indicates a condition toachieve low-profileness and correct astigmatism and field curvatureproperly, provided that the fifth lens has negative refractive power andthe sixth lens has positive refractive power. If the value is above theupper limit of the conditional expression (4), the negative refractivepower of the fifth lens would be too strong to shorten the total tracklength. On the other hand, if the value is below the lower limit of theconditional expression (4), the negative refractive power of the fifthlens would be too weak to correct astigmatism and field curvature.

If the fifth lens has negative refractive power and the sixth lens haspositive refractive power, preferably the imaging lens according to thepresent invention satisfies a conditional expression (5) below:

1.0<f6/f<3.0   (5)

where

-   -   f: focal length of the overall optical system of the imaging        lens, and    -   f6: focal length of the sixth lens.

The conditional expression (5) defines an appropriate range for theratio of the focal length of the sixth lens to the focal length of theoverall optical system of the imaging lens, and indicates a condition toachieve low-profileness and correct spherical aberrations and distortionproperly, provided that the fifth lens has negative refractive power andthe sixth lens has positive refractive power. If the value is above theupper limit of the conditional expression (5), the positive refractivepower of the sixth lens would be too weak to shorten the total tracklength. On the other hand, if the value is below the lower limit of theconditional expression (5), the positive refractive power of the sixthlens would be too strong and spherical aberrations and distortion wouldincrease, thereby making it difficult to correct aberrations, though itwould be advantageous in shortening the total track length.

Preferably, the imaging lens according to the present inventionsatisfies conditional expressions (6) to (8) below:

20<vd1−vd2<40   (6)

40<vd3<75   (7)

40<vd7<75   (8)

where

vd1: Abbe number of the first lens at d-ray,

vd2: Abbe number of the second lens at d-ray,

vd3: Abbe number of the third lens at d-ray, and

vd7: Abbe number of the seventh lens at d-ray.

The conditional expression (6) defines an appropriate range for thedifference between the Abbe numbers of the first and second lenses atd-ray, the conditional expression (7) defines an appropriate range forthe Abbe number of the third lens at d-ray, and the conditionalexpression (8) defines an appropriate range for the Abbe number of theseventh lens at d-ray, and these conditional expressions indicateconditions to correct chromatic aberrations properly. The conditionalexpression (6) suggests that when low-dispersion material is used forthe first lens and high-dispersion material is used for the second lens,chromatic aberrations which occur on the first lens are correctedproperly. The conditional expressions (7) and (8) suggest thatlow-dispersion material is used for the third lens and seventh lens,chromatic aberrations of magnification are suppressed.

If the fifth lens has positive refractive power, preferably the imaginglens according to the present invention satisfies conditionalexpressions (9) and (10) below:

40<vd4<75   (9)

20<|vd5−vd6|<40   (10)

where

vd4: Abbe number of the fourth lens at d-ray,

vd5: Abbe number of the fifth lens at d-ray, and

vd6: Abbe number of the sixth lens at d-ray.

The conditional expression (9) defines an appropriate range for the Abbenumber of the fourth lens at d-ray, and indicates a condition to correctchromatic aberrations properly. When low-dispersion material is used forthe fourth lens, chromatic aberrations of magnification are suppressed.

The conditional expression (10) defines an appropriate range for thedifference between the Abbe numbers of the fifth lens and the sixth lensat d-ray, and indicates a condition to correct chromatic aberrationsproperly. When low-dispersion material and high-dispersion material arecombined for the fifth lens and the sixth lens, chromatic aberrations ofmagnification and axial chromatic aberrations are suppressed.

If the fifth lens has negative refractive power, preferably the imaginglens according to the present invention satisfies conditionalexpressions (11) and (12) below:

20<|vd4−vd51<40   (11)

40<vd6<75   (12)

where

vd4: Abbe number of the fourth lens at d-ray,

vd5: Abbe number of the fifth lens at d-ray, and

vd6: Abbe number of the sixth lens at d-ray.

The conditional expression (11) defines an appropriate range for thedifference between the Abbe numbers of the fourth lens and the fifthlens at d-ray, and indicates a condition to correct chromaticaberrations properly. When low-dispersion material and high-dispersionmaterial are combined for the fourth lens and the fifth lens, chromaticaberrations of magnification and axial chromatic aberrations aresuppressed.

The conditional expression (12) defines an appropriate range for theAbbe number of the sixth lens at d-ray, and indicates a condition tocorrect chromatic aberrations properly. When low-dispersion material isused for the sixth lens, chromatic aberrations of magnification aresuppressed.

The conditional expressions (6) to (12) suggest that inexpensive plasticmaterials may be used for the constituent lenses. This makes it easy toreduce the cost of the imaging lens.

Preferably, the imaging lens according to the present inventionsatisfies conditional expressions (13) and (14) below:

1.0<TTL/f<1.35   (13)

TTL/2ih<1.0   (14)

where

-   -   f: focal length of the overall optical system of the imaging        lens,    -   TTL: distance on the optical axis from an object-side surface of        an optical element located nearest to the object to the image        plane with a filter, etc. removed (total track length), and    -   ih: maximum image height.

The conditional expression (13) defines an appropriate range for theratio of total track length to the focal length of the overall opticalsystem of the imaging lens, and indicates a condition to achievelow-profileness and correct various aberrations properly. If the valueis above the upper limit of the conditional expression (13), the totaltrack length would be too long to achieve low-profileness, though thefreedom in the shape of each constituent lens would increase, therebymaking it easier to correct various aberrations. On the other hand, ifthe value is below the lower limit of the conditional expression (13),the total track length would be too short and the freedom in the shapeof each constituent lens would decrease, thereby making it difficult tocorrect various aberrations.

The conditional expression (14) defines an appropriate relation betweentotal track length and maximum image height, and indicates a conditionto make the imaging lens low-profile. When the value is below the upperlimit of the conditional expression (14), the total track length isshorter than the diagonal length of the effective imaging plane of theimage sensor, and the imaging lens can meet the recent demand forlow-profileness.

If the fifth lens has positive refractive power and the sixth lens hasnegative refractive power, preferably the imaging lens according to thepresent invention satisfies conditional expressions (15) and (16) below:

0.4<f345/f<1.2   (15)

−1.0<f67/f<−0.3   (16)

where

-   -   f: focal length of the overall optical system of the imaging        lens,    -   f345: composite focal length of the third lens, the fourth lens,        and the fifth lens, and    -   f67: composite focal length of the sixth lens and the seventh        lens.

The conditional expression (15) defines an appropriate range for theratio of the composite focal length of the third, fourth, and fifthlenses to the focal length of the overall optical system of the imaginglens, and indicates a condition to achieve low-profileness and correctspherical aberrations and coma aberrations properly. If the value isabove the upper limit of the conditional expression (15), the compositerefractive power of the third, fourth, and fifth lenses would be tooweak to shorten the total track length. On the other hand, if the valueis below the lower limit of the conditional expression (15), thecomposite refractive power of the third, fourth, and fifth lenses wouldbe too strong and spherical aberrations and coma aberrations wouldincrease, thereby making it difficult to correct aberrations, though itwould be advantageous in shortening the total track length.

The conditional expression (16) defines an appropriate range for theratio of the composite focal length of the sixth and seventh lenses tothe focal length of the overall optical system of the imaging lens, andindicates a condition to achieve low-profileness and correct chromaticaberrations properly. If the value is above the upper limit of theconditional expression (16), the composite negative refractive power ofthe sixth and seventh lenses would be too strong to shorten the totaltrack length. On the other hand, if the value is below the lower limitof the conditional expression (16), the composite negative refractivepower of the sixth and seventh lenses would be too weak to correctchromatic aberrations properly. When the conditional expressions (15)and (16) are satisfied, low-profileness is ensured and aberrations whichoccur on the third, fourth, and fifth lenses are corrected by the sixthand seventh lenses properly.

If the fifth lens has negative refractive power and the sixth lens haspositive refractive power, preferably the imaging lens according to thepresent invention satisfies conditional expressions (17) and (18) below:

2.0<f345/f<8.0   (17)

−6.0<f67/f<−2.0   (18)

where

-   -   f: focal length of the overall optical system of the imaging        lens,    -   f345: composite focal length of the third lens, the fourth lens,        and the fifth lens, and    -   f67: composite focal length of the sixth lens and the seventh        lens.

The conditional expression (17) defines an appropriate range for theratio of the composite focal length of the third, fourth, and fifthlenses to the focal length of the overall optical system of the imaginglens, and indicates a condition to achieve low-profileness and correctspherical aberrations and coma aberrations properly. If the value isabove the upper limit of the conditional expression (17), the compositerefractive power of the third, fourth, and fifth lenses would be tooweak to shorten the total track length. On the other hand, if the valueis below the lower limit of the conditional expression (17), thecomposite refractive power of the third, fourth, and fifth lenses wouldbe too strong and spherical aberrations and coma aberrations wouldincrease, thereby making it difficult to correct aberrations, though itwould be advantageous in shortening the total track length.

The conditional expression (18) defines an appropriate range for theratio of the composite focal length of the sixth and seventh lenses tothe focal length of the overall optical system of the imaging lens, andindicates a condition to achieve low-profileness and correct chromaticaberrations properly. If the value is above the upper limit of theconditional expression (18), the composite negative refractive power ofthe sixth and seventh lenses would be too strong to shorten the totaltrack length. On the other hand, if the value is below the lower limitof the conditional expression (18), the composite negative refractivepower of the sixth and seventh lenses would be too weak to correctchromatic aberrations properly. When the conditional expressions (17)and (18) are satisfied, low-profileness is ensured and opticalperformance is improved.

Preferably, in the imaging lens according to present invention, thefifth lens has a meniscus shape with a concave surface on the objectside. When the fifth lens has a meniscus shape with a concave surface onthe object side, off-axial rays can exit the fifth lens at a small exitangle and easily enter the sixth lens, so that off-axial aberrations,mainly astigmatism and field curvature, are corrected properly.

If the fifth lens has positive refractive power, preferably the imaginglens according to the present invention satisfies a conditionalexpression (19) below:

0.8<(r9+r10)/(r9−r10)<2.5   (19)

where

-   -   r9: curvature radius of the object-side surface of the fifth        lens, and    -   r10: curvature radius of the image-side surface of the fifth        lens.

The conditional expression (19) defines an appropriate range for theratio of the sum of the curvature radii of the object-side andimage-side surfaces of the fifth lens to the difference between thecurvature radii, and indicates a condition to correct variousaberrations properly, provided that the fifth lens has positiverefractive power. If the value is above the upper limit of theconditional expression (19), the refractive power of the image-sidesurface of the fifth lens would be too weak to suppress high-orderaberrations such as field curvature. On the other hand, if the value isbelow the lower limit of the conditional expression (19), the refractivepower of the image-side surface of the fifth lens would be too strong tocorrect distortion in the peripheral area.

If the fifth lens has negative refractive power, preferably the imaginglens according to the present invention satisfies a conditionalexpression (20) below:

−20.0<(r9+r10)/(r9−r10)<−4.0   (

where

-   -   r9: curvature radius of the object-side surface of the fifth        lens, and    -   r10: curvature radius of the image-side surface of the fifth        lens.

The conditional expression (20) defines an appropriate range for theratio of the sum of the curvature radii of the object-side andimage-side surfaces of the fifth lens to the difference between thecurvature radii, and indicates a condition to correct variousaberrations properly, provided that the fifth lens has negativerefractive power. If the value is above the upper limit of theconditional expression (20), the refractive power of the object-sidesurface of the fifth lens would be too strong to suppress astigmatismand distortion. On the other hand, if the value is below the lower limitof the conditional expression (20), the refractive power of theobject-side surface of the fifth lens would be too weak to correct fieldcurvature and coma aberrations. When the conditional expression (20) issatisfied, it is easier to correct coma aberrations, field curvature,astigmatism, and field curvature.

Preferably, the imaging lens according to the present inventionsatisfies a conditional expression (21) below:

f/EPD<2.40   (21)

where

-   -   f: focal length of the overall optical system of the imaging        lens, and    -   EPD: entrance pupil diameter.

The conditional expression (21) indicates a condition to determine thebrightness of the imaging lens and corresponds to an F-value. When thepixel size is smaller, there is a tendency that the quantity of lightwhich the image sensor takes from the imaging lens tends decreases andthus it is difficult to form a bright image. If the sensitivity of theimage sensor is increased to address this problem, image quality maydeteriorate due to noise, etc. Therefore, as a solution to the problem,it is effective to increase the quantity of light exiting the imaginglens. When the conditional expression (21) is satisfied, the imaginglens can be applied to a recent image sensor with a high pixel density.

Preferably, in the imaging lens according to the present invention, thefirst to seventh lenses are made of plastic material and all lenssurfaces are aspheric. When plastic material is used for all theconstituent lenses, the imaging lens with aspheric lens surfaces can bemass-produced stably at low cost. When all the lens surfaces areaspheric, various aberrations are corrected properly.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic view showing the general configuration of animaging lens in Example 1 according to an embodiment of the presentinvention;

FIG. 2 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 1 according to the embodiment of the presentinvention;

FIG. 3 is a schematic view showing the general configuration of animaging lens in Example 2 according to the embodiment of the presentinvention;

FIG. 4 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 2 according to the embodiment of the presentinvention;

FIG. 5 is a schematic view showing the general configuration of animaging lens in Example 3 according to the embodiment of the presentinvention;

FIG. 6 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 3 according to the embodiment of the presentinvention;

FIG. 7 is a schematic view showing the general configuration of animaging lens in Example 4 according to the embodiment of the presentinvention;

FIG. 8 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 4 according to the embodiment of the presentinvention;

FIG. 9 is a schematic view showing the general configuration of animaging lens in Example 5 according to the embodiment of the presentinvention;

FIG. 10 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 5 according to the embodiment of the presentinvention;

FIG. 11 is a schematic view showing the general configuration of animaging lens in Example 6 according to the embodiment of the presentinvention;

FIG. 12 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 6 according to the embodiment of the presentinvention;

FIG. 13 is a schematic view showing the general configuration of animaging lens in Example 7 according to the embodiment of the presentinvention;

FIG. 14 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 7 according to the embodiment of the presentinvention;

FIG. 15 is a schematic view showing the general configuration of animaging lens in Example 8 according to the embodiment of the presentinvention; and

FIG. 16 shows spherical aberration, astigmatism, and distortion of theimaging lens in Example 8 according to the embodiment of the presentinvention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

Hereinafter, the preferred embodiment of the present invention will bedescribed in detail referring to the accompanying drawings. FIGS. 1, 3,5, 7, 9, 11, 13, and 15 are schematic views showing the generalconfigurations of the imaging lenses in Examples 1 to 8 according tothis embodiment, respectively. Since all these examples have the samebasic lens configuration, the general configuration of an imaging lensaccording to this embodiment is explained below mainly referring to theschematic view of Example 1.

As shown in FIG. 1, the imaging lens according to this embodiment is animaging lens composed of seven constituent lenses which forms an imageof an object on a solid-state image sensor and includes, in order froman object side to an image side, a first lens L1 with positiverefractive power having a convex surface on the object side, a secondlens L2 with negative refractive power, a third lens L3 with positiverefractive power, a fourth lens L4 with negative refractive power, afifth lens L5 with positive refractive power, a sixth lens L6 withnegative refractive power, and a seventh lens L7 as a double-sidedaspheric lens having a concave surface on the image side. Theseconstituent lenses are spaced from each other and the third lens L3 tothe sixth lens L6 each have at least one aspheric surface. The asphericimage-side surface of the seventh lens L7 has pole-change points off anoptical axis X.

A filter IR such as an infrared cut filter is located between theseventh lens L7 and an image plane IMG. The filter IR is omissible. Thevalues of total track length and back focus of the imaging lensaccording to this embodiment are defined to express distances on theoptical axis X in which the filter IR is removed.

An aperture stop ST is located on the object side of the first lens L1.

In this embodiment, the first lens L1 is a biconvex lens having a convexsurface on each of the object and image sides, which has strong positiverefractive power to achieve low-profileness. As for the shape of thefirst lens L1, it only has to have a convex surface on the object side.It may have a meniscus shape with a convex surface on the object side asin Examples 3, 4, 5, 7, and 8 shown in FIGS. 5, 7, 9, 13, and 15,respectively.

The second lens L2 is a meniscus double-sided aspheric lens withnegative refractive power having a convex surface on the object side,which properly corrects spherical aberrations and chromatic aberrationswhich occur on the first lens L1. The second lens L2 should at leasthave negative refractive power. It may have a biconcave shape with aconcave surface on each of the object and image sides as in Example 4shown in FIG. 7 or may have a meniscus shape with a concave surface onthe object side as in Example 5 shown in FIG. 9.

The third lens L3 is a biconvex double-sided aspheric lens with positiverefractive power having a convex surface on each of the object andimages sides. The shape of the third lens L3 is not limited to abiconvex shape. Instead, it may be a meniscus shape with a concavesurface on the object side as in Example 3 shown in FIG. 5 or a meniscusshape with a convex surface on the object side as in Example 5 shown inFIG. 9 or a biconcave shape with a concave surface on each of the objectand image sides as in Example 8 shown in FIG. 15. The refractive powerof the third lens L3 is not limited to positive refractive power. InExample 8 shown in FIG. 15, the third lens L3 has negative refractivepower.

The fourth lens L4 is a meniscus double-sided aspheric lens withnegative refractive power having a concave surface on the object side.The refractive power of the fourth lens L4 is not limited to negativerefractive power. In Example 5 shown in FIG. 9, the fourth lens L4 is ameniscus lens with positive refractive power having a convex surface onthe object side and in Example 8 shown in FIG. 15, the fourth lens L4 isa biconvex lens with positive refractive power having a convex surfaceon each of the object and image sides.

The fifth lens L5 is a meniscus double-sided aspheric lens with positiverefractive power having a concave surface on the object side. Therefractive power of the fifth lens L5 is not limited to positiverefractive power. In Examples 7 and 8 shown in FIGS. 13 and 15,respectively, the fifth lens L5 is a meniscus lens with negativerefractive power having a concave surface on the object side.

The sixth lens L6 is a biconcave double-sided aspheric lens withnegative refractive power having a concave surface on each of the objectand image sides. The refractive power of the sixth lens L6 is notlimited to negative refractive power. In Examples 7 and 8 shown in FIGS.13 and 15 respectively, the sixth lens L6 is a meniscus lens withpositive refractive power having a convex surface on the object side.

The third lens L3 to the sixth lens L6 have appropriate positive ornegative refractive power and their surfaces are aspheric, so that theimaging lens is low-profile and corrects off-axial aberrations such asastigmatism, field curvature, and distortion properly.

The seventh lens L7 is a biconcave double-sided aspheric lens withnegative refractive power having a concave surface on each of the objectand image sides. The both aspheric surfaces correct sphericalaberrations, and field curvature and distortion in the peripheral area.Since the image-side surface of the seventh lens L7 is an asphericsurface with pole-change points, the angle of rays incident on the imagesensor IMG is controlled appropriately. The shape of the seventh lens L7is not limited to a biconcave shape. In Examples 3 and 7 shown in FIGS.5 and 13 respectively, the seventh lens L7 has a meniscus shape with aconvex surface on the object side.

In the imaging lens composed of seven constituent lenses according tothis embodiment, when the first lens L1 and the second lens L2 areassumed to constitute one group, their composite refractive power ispositive; when the third lens L3, the fourth lens L4, and the fifth lensL5 are assumed to constitute one group, their composite refractive poweris positive; and when the sixth lens L6 and the seventh lens L7 areassumed to constitute one group, their composite refractive power isnegative. Thus, positive, positive, and negative refractive power lensgroups are arranged in order from the object side, making a so-calledtelephoto type power arrangement which is advantageous in making theimaging lens low-profile.

In the imaging lens according to this embodiment, the aperture stop STis located on the object side of the first lens L1. Therefore, the exitpupil is remote from the image plane IMG, which ensures telecentricityand prevents a decline in the quantity of light in the peripheral areaof the image.

When all the constituent lenses of the imaging lens according to thisembodiment are made of plastic material, the manufacturing process iseasier and the imaging lens can be mass-produced at low cost. All thelens surfaces have appropriate aspheric shapes to correct variousaberrations more properly.

In the imaging lens according to this embodiment, if the fifth lens L5has positive refractive power and the sixth lens L6 has negativerefractive power, when conditional expressions (1) to (3), conditionalexpressions (6) to (10), conditional expressions (13) to (16), andconditional expressions (19) and (21) below are satisfied, advantageouseffects are brought about. If the fifth lens L5 has negative refractivepower and the sixth lens L6 has positive refractive power, when aconditional expression (1), conditional expressions (4) to (8),conditional expressions (11) to (14), and conditional expressions (17),(18), (20), and (21) below are satisfies, advantageous effects arebrought about.

−1.0<f1/f2<−0.15   (1)

0.5<f5/f<1.5   (2)

−8.0<f6/f<−1.0   (3)

−20<f5/f<−1.0   (4)

1.0<f6/f<3.0   (5)

20<vd1−vd2<40   (6)

40<vd3<75   (7)

40<vd7<75   (8)

40<vd4<75   (9)

20<|vd5−vd6|<40   (10)

20<|vd4−vd5|<40   (11)

40<vd6<75   (12)

1.0<TTL/f<1.35   (13)

TTL/2ih<1.0   (14)

0.4<f345/f<1.2   (15)

−1.0<f67/f<−0.3   (16)

2.0<f345/f<8.0   (17)

−6.0<f67/f<−2.0   (18)

0.8<(r9+r10)/(r9−r10)<2.5   (19)

−20.0<(r9+r10)/(r9−r10)<−4.0   (20)

f/EPD<2.40   (21)

where

-   -   f: focal length of the overall optical system of the imaging        lens,    -   f1: focal length of the first lens L1,    -   f2: focal length of the second lens L2,    -   f5: focal length of the fifth lens L5,    -   f6: focal length of the sixth lens L6,    -   f345: composite focal length of the third lens L3, the fourth        lens L4, and the fifth lens L5,    -   f67: composite focal length of the sixth lens L6 and the seventh        lens L7,    -   vd1: Abbe number of the first lens L1 at d-ray,    -   vd2: Abbe number of the second lens L2 at d-ray,    -   vd3: Abbe number of the third lens L3 at d-ray,    -   vd4: Abbe number of the fourth lens L4 at d-ray,    -   vd5: Abbe number of the fifth lens L5 at d-ray,    -   vd6: Abbe number of the sixth lens L6 at d-ray,    -   vd7: Abbe number of the seventh lens L7 at d-ray,    -   r9: curvature radius of the object-side surface of the fifth        lens L5,    -   r10: curvature radius of the image-side surface of the fifth        lens L5,    -   TTL: distance on the optical axis X from the object-side surface        of an optical element located nearest to the object to the image        plane IMG with the filter IR removed (total track length),    -   ih: maximum image height, and    -   EPD: entrance pupil diameter.

In the imaging lens according to this embodiment, if the fifth lens L5has positive refractive power and the sixth lens L6 has negativerefractive power, when conditional expressions (1a) to (3a), conditionalexpressions (6a) to (10a), conditional expressions (13a) to (16a), andconditional expressions (19a) and (21a) below are satisfied, moreadvantageous effects are brought about. If the fifth lens L5 hasnegative refractive power and the sixth lens L6 has positive refractivepower, when a conditional expression (1a), conditional expressions (4a)to (8a), conditional expressions (11a) to (14a), and conditionalexpressions (17a), (18a), (20a), and (21a) below are satisfied, moreadvantageous effects are brought about.

−0.80<f1/f2<−0.20   (1a)

0.7<f5/f<1.3   (2a)

−6.5<f6/f<−2.0   (3a)

−19<f5/f<−2.0   (4a)

1.4<f6/f<2.4   (5a)

24<vd1−vd2<36   (6a)

45<vd3<65   (7a)

45<vd7<65   (8a)

45<vd4<65   (9a)

24<|vd5−vd6|<36   (10a)

24<|vd4−vd5|<36   (11a)

45<vd6<65   (12a)

1.1<TTL/f<1.32   (13a)

TTL/2ih<0.95   (14a)

0.6<f345/f<1.0   (15a)

−0.8<f67/f<−0.4   (16a)

3.0<f345/f<7.0   (17a)

−5.0<f67/f<−2.5   (18a)

0.9<(r9+r10)/(r9−r10)<2.3   (19a)

−19.0<(r9+r10)/(r9−r10)<−5.0   (20a)

f/EPD<2.20.   (21a)

The signs in the above conditional expressions have the same meanings asthose in the preceding paragraph.

In the imaging lens according to this embodiment, if the fifth lens L5has positive refractive power and the sixth lens L6 has negativerefractive power, when conditional expressions (1b) to (3b), conditionalexpressions (6b) to (10b), conditional expressions (13b) to (16b), andconditional expressions (19b) and (21b) below are satisfied,particularly advantageous effects are brought about. If the fifth lensL5 has negative refractive power and the sixth lens L6 has positiverefractive power, when a conditional expression (1b), conditionalexpressions (4b) to (8b), conditional expressions (lib) to (14b), andconditional expressions (17b), (18b), (20b), and (21b) below aresatisfied, particularly advantageous effects are brought about.

−0.63≤f1/f2≤−0.31   (1b)

0.92≤f5/f≤1.14   (2b)

−5.07≤f6/f≤−2.98   (3b)

−17.70≤f5/f≤−3.36   (4b)

1.77≤f6/f1.84   (5b)

28<vd1−vd2<34   (6b)

50<vd3<60   (7b)

50<vd7<60   (8b)

50<vd4<60   (9b)

28<|vd5−vd61<32   (10b)

28<|vd4−vd51<34   (11b)

50<vd6<60   (12b)

1.23≤TTL/f≤1.28   (13b)

TTL/2ih≤0.89   (14b)

0.78≤f345/f≤0.88   (15b)

−0.67≤f67/f≤−0.59   (16b)

4.11≤f345/f≤6.30   (17b)

−4.00≤f67/f≤−3.16   (18b)

0.97≤(r9+r10)/(r9−r10)≤2.10   (19b)

−17.23≤(r9+r10)/(r9−r10)≤−6.98   (20b)

f/EPD2.08   (21b)

The signs in the above conditional expressions have the same meanings asthose in the paragraph before the preceding paragraph.

In this embodiment, all the lens surfaces are aspheric. The asphericshapes of these lens surfaces are expressed by Equation 1, where Zdenotes an axis in the optical axis direction, H denotes a heightperpendicular to the optical axis, k denotes a conic constant, and A4,A6, A8, A10, A12, A14, and A16 denote aspheric surface coefficients.

$\begin{matrix}{Z = {\frac{\frac{H^{2}}{R}}{1 + \sqrt{1 - {\left( {k + 1} \right)\frac{H^{2}}{R^{2}}}}} + {A_{4}H^{4}} + {A_{6}H^{6}} + {A_{8}H^{8}} + {A_{10}H^{10}} + {A_{12}H^{12}} + {A_{14}H^{14}} + {A_{16}H^{16}}}} & {{Equation}\mspace{14mu} 1}\end{matrix}$

Next, examples of the imaging lens according to this embodiment will beexplained. In each example, f denotes the focal length of the overalloptical system of the imaging lens, Fno denotes an F-number, ω denotes ahalf field of view, ih denotes a maximum image height, TTL denotes totaltrack length. i denotes a surface number counted from the object side, rdenotes a curvature radius, d denotes the distance on the optical axis Xbetween lens surfaces (surface distance), Nd denotes a refractive indexat d-ray (reference wavelength), and vd denotes an Abbe number at d-ray.As for aspheric surfaces, an asterisk (*) after surface number iindicates that the surface concerned is an aspheric surface.

EXAMPLE 1

The basic lens data of Example 1 is shown below in Table 1.

TABLE 1 Example 1 in mm f = 6.68 Fno = 1.64 ω(°) = 37.2 ih = 5.06 TTL =8.52 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface Infinity Infinity 1(Stop) Infinity −0.760  2* 3.162 1.092 1.5438 55.57  3* −77.658 0.025 4* 4.406 0.351 1.6391 23.25  5* 2.552 0.864  6* 34.655 0.609 1.534855.66  7* −17.567 0.025  8* −30.731 0.686 1.5348 55.66  9* −38.000 0.61410* −11.066 0.642 1.5348 55.66 11* −2.601 0.025 12* −14.102 1.267 1.614225.58 13* 99.000 0.469 14* −99.000 0.687 1.5348 55.66 15* 2.923 0.335 16Infinity 0.210 1.5168 64.20 17 Infinity 0.695 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 5.61 (=f1) 2 4−10.25 (=f2) 3 6 21.89 (=f3) 4 8 −310.57 (=f4) 5 10 6.20 (=f5) 6 12−20.01 (=f6) 7 14 −5.30 (=f7) Lens Composite Focal Length 3rd Lens-5thLens 5.19 (=f345) 6th Lens-7th Lens −3.94 (=f67) Aspheric Surface Data2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface 7th Surface8th Surface k 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A4 1.299E−03 4.550E−03 −2.475E−02  −3.225E−02 −3.982E−03  −3.145E−03  −6.430E−03  A6 −5.531E−04  2.091E−03 1.157E−021.215E−02 −2.194E−03  −2.506E−03  −3.547E−08  A8 3.058E−04 −7.995E−04 −3.278E−03  −3.337E−03  2.510E−04 1.678E−04 5.738E−05 A10 −3.081E−05 6.345E−05 3.003E−04 3.750E−04 −6.792E−05  −1.973E−05  0.000E+00 A120.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00A14 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 A16 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 9th Surface 10th Surface 11th Surface 12th Surface13th Surface 14th Surface 15th Surface k 0.000E+00 0.000E+00 −3.149E+00 0.000E+00 0.000E+00 0.000E+00 −6.629E+00 A4 −8.923E−03  −5.363E−03 8.674E−05 4.862E−03 5.257E−03 −2.402E−02  −1.964E−02 A6 −8.478E−04 2.890E−03 2.087E−03 −6.707E−04  −4.149E−03  9.619E−04  2.664E−03 A8−4.465E−05  −1.014E−03  −5.790E−04  −9.472E−04  8.861E−04 3.871E−04−2.455E−04 A10 0.000E+00 6.498E−05 4.455E−05 3.047E−04 −1.126E−04 −5.234E−05   1.429E−05 A12 0.000E+00 0.000E+00 0.000E+00 −4.211E−05 8.775E−06 2.665E−06 −4.629E−07 A14 0.000E+00 0.000E+00 0.000E+002.145E−06 −3.873E−07  −5.661E−08   6.229E−09 A16 0.000E+00 0.000E+000.000E+00 0.000E+00 7.362E−09 3.397E−10 −2.369E−13

In the imaging lens in Example 1, the fifth lens L5 has positiverefractive power and the sixth lens L6 has negative refractive power. Asshown in Table 9, the imaging lens satisfies conditional expressions (1)to (3), conditional expressions (6) to (10), conditional expressions(13) to (16), and conditional expressions (19) and (21).

FIG. 2 shows spherical aberration (mm), astigmatism (mm), and distortion(%) of the imaging lens in Example 1. The spherical aberration diagramshows the amount of aberration at wavelengths of F-ray (486 nm), d-ray(588 nm), and C-ray (656 nm). The astigmatism diagram shows the amountof aberration at d-ray on sagittal image surface S and the amount ofaberration at d-ray on tangential image surface T (the same is true forFIGS. 4, 6, 8, 10, 12, 14, and 16). As shown in FIG. 2, each aberrationis corrected properly.

EXAMPLE 2

The basic lens data of Example 2 is shown below in Table 2.

TABLE 2 Example 2 in mm f = 7.24 Fno = 1.78 ω(°) = 35.0 ih = 5.06 TTL =8.98 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface) Infinity Infinity 1(Stop) Infinity −0.737  2* 3.194 1.306 1.5438 55.57  3* −99.000 0.025 4* 4.434 0.336 1.6391 23.25  5* 2.572 0.899  6* 61.967 0.537 1.534855.66  7* −18.462 0.025  8* 99.000 0.643 1.5348 55.66  9* 84.000 0.70910* −12.706 0.590 1.5348 55.66 11* −3.032 0.025 12* −11.488 1.497 1.614225.58 13* −44.493 0.417 14* −99.000 0.780 1.5348 55.66 15* 3.131 0.34016 Infinity 0.210 1.5168 64.20 17 Infinity 0.713 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 5.72 (=f1) 2 4−10.31 (=f2) 3 6 26.66 (=f3) 4 8 −1052.35 (=f4) 5 10 7.29 (=f5) 6 12−25.66 (=f6) 7 14 −5.66 (=f7) Lens Composite Focal Length 3rd Lens-5thLens 6.07 (=f345) 6th Lens-7th Lens −4.33 (=f67) Aspheric Surface Data2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface 7th Surface8th Surface k 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A4 1.211E−03 4.682E−03 −2.511E−02  −3.283E−02 −3.311E−03  −2.853E−03  −6.946E−03  A6 −6.238E−04  1.880E−03 1.163E−021.227E−02 −2.017E−03  −2.357E−03  −9.364E−05  A8 2.808E−04 −8.340E−04 −3.260E−03  −3.279E−03  2.197E−04 1.569E−04 5.120E−05 A10 −3.399E−05 6.919E−05 3.051E−04 3.588E−04 −6.487E−05  −2.318E−05  0.000E+00 A120.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00A14 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 A16 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 9th Surface 10th Surface 11th Surface 12th Surface13th Surface 14th Surface 15th Surface k 0.000E+00 0.000E+00 −3.100E+00 0.000E+00 0.000E+00 0.000E+00 −6.544E+00 A4 −9.118E−03  −6.338E−03 1.866E−03 6.205E−03 6.366E−03 −2.394E−02  −1.926E−02 A6 −6.852E−04 3.004E−03 1.891E−03 −5.199E−04  −4.132E−03  9.367E−04  2.621E−03 A8−4.378E−05  −9.952E−04  −6.108E−04  −9.594E−04  8.854E−04 3.871E−04−2.440E−04 A10 0.000E+00 6.164E−05 4.524E−05 3.024E−04 −1.129E−04 −5.232E−05   1.436E−05 A12 0.000E+00 0.000E+00 0.000E+00 −4.213E−05 8.766E−06 2.667E−06 −4.627E−07 A14 0.000E+00 0.000E+00 0.000E+002.160E−06 −3.874E−07  −5.647E−08   6.113E−09 A16 0.000E+00 0.000E+000.000E+00 0.000E+00 7.450E−09 3.325E−10  0.000E+00

In the imaging lens in Example 2, the fifth lens L5 has positiverefractive power and the sixth lens L6 has negative refractive power. Asshown in Table 9, the imaging lens satisfies conditional expressions (1)to (3), conditional expressions (6) to (10), conditional expressions(13) to (16), and conditional expressions (19) and (21).

FIG. 4 shows spherical aberration (mm), astigmatism (mm), and distortion(%) of the imaging lens in Example 2. As shown in FIG. 4, eachaberration is corrected properly.

EXAMPLE 3

The basic lens data of Example 3 is shown below in Table 3.

TABLE 3 Example 3 in mm f = 7.04 Fno = 1.73 ω(°) = 35.5 ih = 5.06 TTL =8.69 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface) Infinity Infinity 1(Stop) Infinity −0.771  2* 3.054 1.031 1.5438 55.57  3* 100.000 0.030 4* 3.512 0.300 1.6349 23.97  5* 2.224 0.893  6* −100.000 0.584 1.534855.66  7* −8.285 0.093  8* −100.000 0.649 1.5348 55.66  9* 100.000 0.83210* −8.231 0.611 1.5438 55.57 11* −2.927 0.033 12* −17.671 1.206 1.614225.58 13* −100.000 0.454 14* 100.000 0.728 1.5348 55.66 15* 2.976 0.34016 Infinity 0.210 1.5168 64.20 17 Infinity 0.763 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 5.77 (=f1) 2 4−10.50 (=f2) 3 6 16.85 (=f3) 4 8 −93.39 (=f4) 5 10 8.03 (=f5) 6 12−35.14 (=f6) 7 14 −5.75 (=f7) Lens Composite Focal Length 3rd Lens-5thLens 6.19 (=f345) 6th Lens-7th Lens −4.73 (=f67) Aspheric Surface Data2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface 7th Surface8th Surface k 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A4 2.495E−03 1.139E−03 −4.195E−02  −4.764E−02 −2.266E−03  −1.210E−02  −2.148E−02  A6 −4.970E−04  1.167E−03 1.265E−021.290E−02 −2.394E−03  −1.613E−04  9.998E−04 A8 1.320E−04 −2.268E−04 −2.260E−03  −2.370E−03  1.543E−04 −1.069E−04  2.304E−04 A10 −2.029E−06 9.859E−06 1.550E−04 1.394E−04 −7.792E−06  6.624E−05 0.000E+00 A120.000E+00 0.000E+00 0.000E+00 8.605E−06 0.000E+00 0.000E+00 0.000E+00A14 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 A16 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 9th Surface 10th Surface 11th Surface 12th Surface13th Surface 14th Surface 15th Surface k 0.000E+00 0.000E+00 −1.967E+00 0.000E+00 0.000E+00 0.000E+00 −6.154E+00 A4 −1.522E−02  −6.239E−03 4.188E−03 3.461E−03 6.455E−03 −2.567E−02  −1.942E−02 A6 −3.727E−04 3.258E−03 1.782E−03 7.290E−05 −4.205E−03  9.424E−04  2.521E−03 A8−8.733E−05  −9.653E−04  −5.684E−04  −1.059E−03  8.860E−04 3.860E−04−2.351E−04 A10 0.000E+00 6.283E−05 4.266E−05 3.034E−04 −1.140E−04 −5.207E−05   1.410E−05 A12 0.000E+00 0.000E+00 0.000E+00 −4.064E−05 8.812E−06 2.691E−06 −4.650E−07 A14 0.000E+00 0.000E+00 0.000E+002.044E−06 −3.821E−07  −5.753E−08   6.292E−09 A16 0.000E+00 0.000E+000.000E+00 0.000E+00 7.291E−09 3.131E−10  0.000E+00

In the imaging lens in Example 3, the fifth lens L5 has positiverefractive power and the sixth lens L6 has negative refractive power. Asshown in Table 9, the imaging lens satisfies conditional expressions (1)to (3), conditional expressions (6) to (10), conditional expressions(13) to (16), and conditional expressions (19) and (21).

FIG. 6 shows spherical aberration (mm), astigmatism (mm), and distortion(%) of the imaging lens in Example 3. As shown in FIG. 6, eachaberration is corrected properly.

EXAMPLE 4

The basic lens data of Example 4 is shown below in Table 4.

TABLE 4 Example 4 in mm f = 7.07 Fno = 2.08 ω(°) = 35.5 ih = 5.06 TTL =8.74 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface Infinity Infinity 1(Stop) Infinity −0.503  2* 3.073 1.267 1.5438 55.57  3* 22.871 0.340  4*−10.326 0.260 1.6391 23.25  5* 17.895 0.386  6* 9.119 0.424 1.5348 55.66 7* −31.044 0.175  8* −236.297 0.545 1.5348 55.66  9* 35.694 0.883 10*−9.388 0.688 1.5438 55.57 11* −2.967 0.030 12* −20.276 1.150 1.614225.58 13* −264.821 0.836 14* −119.618 0.651 1.5348 55.66 15* 3.022 0.34016 Infinity 0.210 1.5168 64.20 17 Infinity 0.631 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 6.38 (=f1) 2 4−10.21 (=f2) 3 6 13.23 (=f3) 4 8 −57.94 (=f4) 5 10 7.69 (=f5) 6 12−35.81 (=f6) 7 14 −5.50 (=f7) Lens Composite Focal Length 3rd Lens-5thLens 5.86 (=f345) 6th Lens-7th Lens −4.55 (=f67) Aspheric Surface Data2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface 7th Surface8th Surface k 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A4 2.812E−04 4.073E−03 3.229E−02 2.923E−02−8.377E−03  −2.600E−03  −8.781E−03  A6 −1.297E−05  −5.890E−04 −1.288E−02  −1.199E−02  −3.358E−03  −2.397E−03  −1.457E−04  A8 1.450E−04−5.893E−04  2.540E−03 3.062E−03 2.511E−04 1.666E−04 7.783E−05 A10−5.933E−05  −4.393E−05  −3.411E−04  −2.729E−04  5.484E−05 9.113E−050.000E+00 A12 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A14 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 0.000E+00 A16 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 0.000E+00 0.000E+00 9th Surface 10th Surface 11thSurface 12th Surface 13th Surface 14th Surface 15th Surface k 0.000E+000.000E+00 −2.471E+00  0.000E+00 0.000E+00 0.000E+00 −6.051E+00 A4−1.142E−02  −5.936E−03  1.218E−03 4.643E−03 4.069E−03 −2.814E−02 −1.968E−02 A6 −3.945E−04  3.391E−03 1.616E−03 −6.900E−04  −4.052E−03 8.469E−04  2.597E−03 A8 −1.944E−04  −9.977E−04  −6.517E−04  −9.624E−04 8.739E−04 3.958E−04 −2.406E−04 A10 0.000E+00 6.473E−05 5.661E−053.045E−04 −1.136E−04  −5.176E−05   1.426E−05 A12 0.000E+00 0.000E+000.000E+00 −4.164E−05  8.695E−06 2.678E−06 −4.678E−07 A14 0.000E+000.000E+00 0.000E+00 2.097E−06 −3.760E−07  −5.547E−08   6.364E−09 A160.000E+00 0.000E+00 0.000E+00 0.000E+00 7.528E−09 1.932E−10  0.000E+00

In the imaging lens in Example 4, the fifth lens L5 has positiverefractive power and the sixth lens L6 has negative refractive power. Asshown in Table 9, the imaging lens satisfies conditional expressions (1)to (3), conditional expressions (6) to (10), conditional expressions(13) to (16), and conditional expressions (19) and (21).

FIG. 8 shows spherical aberration (mm), astigmatism (mm), and distortion(%) of the imaging lens in Example 4. As shown in FIG. 8, eachaberration is corrected properly.

EXAMPLE 5

The basic lens data of Example 5 is shown below in Table 5.

TABLE 5 Example 5 in mm f = 7.07 Fno = 2.08 ω(°) = 35.5 ih = 5.06 TTL =8.74 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface) Infinity Infinity 1(Stop) Infinity −0.763  2* 3.124 1.196 1.5438 55.57  3* 22.290 0.342  4*−6.797 0.260 1.6391 23.25  5* −100.000 0.389  6* 4.544 0.282 1.534855.66  7* 5.738 0.361  8* 9.604 0.713 1.5348 55.66  9* 21.488 0.766 10*−8.892 0.672 1.5438 55.57 11* −3.007 0.030 12* −31.825 1.150 1.614225.58 13* 39.416 0.843 14* −100.000 0.651 1.5348 55.66 15* 3.196 0.34016 Infinity 0.210 1.5168 64.20 17 Infinity 0.608 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 6.54 (=f1) 2 4−11.42 (=f2) 3 6 37.72 (=f3) 4 8 31.81 (=f4) 5 10 8.03 (=f5) 6 12 −28.49(=f6) 7 14 −5.78 (=f7) Lens Composite Focal Length 3rd Lens-5th Lens6.12 (=f345) 6th Lens-7th Lens −4.58 (=f67) Aspheric Surface Data 2ndSurface 3rd Surface 4th Surface 5th Surface 6th Surface 7th Surface 8thSurface k 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 A4 6.774E−04 2.353E−03 3.310E−02 2.990E−02 −7.780E−03 −4.218E−03  −1.063E−02  A6 −2.737E−04  −6.591E−04  −1.296E−02 −1.204E−02  −3.417E−03  −3.030E−03  −2.298E−04  A8 2.628E−04 −4.045E−04 2.525E−03 2.946E−03 1.118E−04 1.352E−04 4.425E−05 A10 −7.102E−05 −5.296E−05  −2.680E−04  −2.065E−04  7.835E−05 7.224E−05 0.000E+00 A120.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00A14 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 A16 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 9th Surface 10th Surface 11th Surface 12th Surface13th Surface 14th Surface 15th Surface k 0.000E+00 0.000E+00 −2.027E+00 0.000E+00 0.000E+00 0.000E+00 −6.107E+00 A4 −1.090E−02  −7.975E−03 6.022E−04 1.995E−03 2.804E−03 −2.777E−02  −2.042E−02 A6 −3.063E−04 3.573E−03 1.601E−03 −5.653E−04  −4.002E−03  8.375E−04  2.641E−03 A8−1.676E−04  −1.026E−03  −6.439E−04  −9.592E−04  8.779E−04 3.958E−04−2.410E−04 A10 0.000E+00 5.987E−05 5.865E−05 3.050E−04 −1.135E−04 −5.174E−05   1.421E−05 A12 0.000E+00 0.000E+00 0.000E+00 −4.153E−05 8.707E−06 2.678E−06 −4.664E−07 A14 0.000E+00 0.000E+00 0.000E+002.095E−06 −3.764E−07  −5.554E−08   6.392E−09 A16 0.000E+00 0.000E+000.000E+00 0.000E+00 7.374E+09 1.926E+10  0.000E+00

In the imaging lens in Example 5, the fifth lens L5 has positiverefractive power and the sixth lens L6 has negative refractive power. Asshown in Table 9, the imaging lens satisfies conditional expressions (1)to (3), conditional expressions (6) to (10), conditional expressions(13) to (16), and conditional expressions (19) and (21).

FIG. 10 shows spherical aberration (mm), astigmatism (mm), anddistortion (%) of the imaging lens in Example 5. As shown in FIG. 10,each aberration is corrected properly.

EXAMPLE 6

The basic lens data of Example 6 is shown below in Table 6.

TABLE 6 Example 6 in mm f = 7.05 Fno = 2.01 ω(°) = 35.5 ih = 5.06 TTL =8.83 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface) Infinity Infinity 1(Stop) Infinity −0.543  2* 3.137 0.974 1.5438 55.57  3* −304.981 0.025 4* 4.311 0.333 1.6391 23.25  5* 2.561 1.037  6* 32.141 0.464 1.534855.66  7* −56.524 0.025  8* −312.099 0.938 1.5348 55.66  9* 134.5410.595 10* 200.000 0.708 1.5348 55.66 11* −3.532 0.025 12* −16.516 1.2181.6142 25.58 13* 60.969 0.761 14* −36.624 0.651 1.5348 55.66 15* 3.3860.340 16 Infinity 0.210 1.5168 64.20 17 Infinity 0.601 (Image Plane)Infinity Constituent Lens Data Lens Start Surface Focal Length 1 2 5.72(=f1) 2 4 −10.66 (=f2) 3 6 38.38 (=f3) 4 8 −175.66 (=f4) 5 10 6.50 (=f5)6 12 −21.03 (=f6) 7 14 −5.76 (=f7) Lens Composite Focal Length 3rdLens-5th Lens 5.96 (=f345) 6th Lens-7th Lens −4.25 (=f67) AsphericSurface Data 2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface7th Surface 8th Surface k 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 0.000E+00 A4 1.961E−03 4.675E−03 −2.514E−02 −3.275E−02  −5.063E−03  −3.506E−03  −6.421E−03  A6 −5.326E−04  1.912E−031.154E−02 1.244E−02 −2.029E−03  −2.380E−03  −1.911E−04  A8 3.341E−04−8.674E−04  −3.234E−03  −3.247E−03  2.071E−04 1.621E−04 4.698E−05 A10−4.656E−05  6.886E−05 3.084E−04 3.823E−04 −6.583E−05  −2.418E−05 0.000E+00 A12 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A14 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 0.000E+00 A16 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 0.000E+00 0.000E+00 9th Surface 10th Surface 11thSurface 12th Surface 13th Surface 14th Surface 15th Surface k 0.000E+000.000E+00 −3.168E+00  0.000E+00 0.000E+00 0.000E+00 −5.344E+00 A4−1.295E−02  −1.118E−02  1.642E−03 5.036E−03 5.811E−03 −2.504E−02 −2.118E−02 A6 −4.765E−04  2.866E−03 1.672E−03 −5.603E−04  −4.154E−03 9.899E−04  2.712E−03 A8 −2.737E−05  −9.384E−04  −6.246E−04  −9.471E−04 8.805E−04 3.887E−04 −2.426E−04 A10 0.000E+00 6.259E−05 4.798E−053.025E−04 −1.129E−04  −5.230E−05   1.430E−05 A12 0.000E+00 0.000E+000.000E+00 −4.211E−05  8.777E−06 2.665E−06 −4.662E−07 A14 0.000E+000.000E+00 0.000E+00 2.131E−06 −3.859E−07  −5.665E−08   6.201E−09 A160.000E+00 0.000E+00 0.000E+00 0.000E+00 7.448E−09 3.334E−10  0.000E+00

In the imaging lens in Example 6, the fifth lens L5 has positiverefractive power and the sixth lens L6 has negative refractive power. Asshown in Table 9, the imaging lens satisfies conditional expressions (1)to (3), conditional expressions (6) to (10), conditional expressions(13) to (16), and conditional expressions (19) and (21).

FIG. 12 shows spherical aberration (mm), astigmatism (mm), anddistortion (%) of the imaging lens in Example 6. As shown in FIG. 12,each aberration is corrected properly.

EXAMPLE 7

The basic lens data of Example 7 is shown below in Table 7.

TABLE 7 Example 7 in mm f = 7.04 Fno = 1.83 ω(°) = 35.5 ih = 5.06 TTL =9.01 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface) Infinity Infinity 1(Stop) Infinity −0.734  2* 3.085 1.190 1.5438 55.57  3* 11.759 0.179  4*3.692 0.260 1.6391 23.25  5* 2.891 0.468  6* 26.089 0.756 1.5348 55.66 7* −5.068 0.252  8* −3.383 1.086 1.6391 23.25  9* −6.318 0.242 10*−4.060 0.638 1.5348 55.66 11* −4.560 0.030 12* 4.809 0.916 1.5348 55.6613* 16.148 0.975 14* 100.000 0.883 1.5348 55.66 15* 3.323 0.400 16Infinity 0.210 1.5168 64.20 17 Infinity 0.595 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 7.34 (=f1) 2 4−23.87 (=f2) 3 6 8.00 (=f3) 4 8 −13.32 (=f4) 5 10 −124.56 (=f5) 6 1212.46 (=f6) 7 14 −6.45 (=f7) Lens Composite Focal Length 3rd Lens-5thLens 28.94 (=f345) 6th Lens-7th Lens −22.25 (=f67) Aspheric Surface Data2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface 7th Surface8th Surface k 0.000E+00 −1.445E+01 −8.301E+00 −6.359E+00  0.000E+00 3.978E+00 −5.383E+00 A4 4.044E−03 −4.974E−03 −3.535E−02 −2.547E−02−1.474E−02 −7.569E−03 −2.332E−02 A6 −3.141E−03  −1.244E−03  2.668E−03 4.308E−03  3.464E−03 −1.310E−03  7.453E−04 A8 3.392E−03  8.003E−03 1.040E−02 −5.864E−04 −7.038E−03 −1.548E−03 −1.404E−03 A10 −1.779E−03 −6.553E−03 −1.003E−02 −1.689E−04  4.593E−03  1.087E−03  8.168E−04 A125.410E−04  2.649E−03  4.498E−03  7.675E−05 −1.819E−03 −2.984E−04−2.744E−04 A14 −8.553E−05  −5.469E−04 −1.043E−03 −2.165E−05  4.294E−04 4.269E−05  4.760E−05 A16 5.707E−06  4.528E−05  9.707E−05  2.370E−06−4.494E−05 −2.475E−06 −2.467E−06 9th Surface 10th Surface 11th Surface12th Surface 13th Surface 14th Surface 15th Surface k 0.000E+000.000E+00 −1.606E+00 −1.659E+01 0.000E+00 0.000E+00 −6.122E−01 A4−5.307E−03  6.152E−03 −1.201E−02  1.017E−02 2.185E−02 −2.464E−02 −3.437E−02 A6 3.277E−04 1.575E−04  2.232E−03 −9.959E−03 −1.282E−02 1.071E−03  4.544E−03 A8 −6.690E−05  2.602E−05  3.140E−04  2.712E−032.998E−03 2.646F−04 −5.099E−04 A10 −2.278E−06  9.558E−07 −1.011E−04−4.412E−04 −4.338E−04  −3.718E−05   4.068E−05 A12 3.451E−06 9.317E−07 8.609E−06  3.639E−05 3.706E−05 1.930E−06 −2.029E−06 A14 6.729E−073.936E−07  1.316E−07 −1.248E−06 −1.702E−06  −3.740E−08   5.488E−08 A160.000E+00 −7.412E−08  −4.845E−08  7.864E−09 3.236E−08 0.000E+00−6.111E−10

In the imaging lens in Example 7, the fifth lens L5 has negativerefractive power and the sixth lens L6 has positive refractive power. Asshown in Table 9, the imaging lens satisfies a conditional expression(1), conditional expressions (4) to (8), conditional expressions (11) to(14), conditional expressions (17), (18), (20), and (21).

FIG. 14 shows spherical aberration (mm), astigmatism (mm), anddistortion (%) of the imaging lens in Example 7. As shown in FIG. 14,each aberration is corrected properly.

EXAMPLE 8

The basic lens data of Example 8 is shown below in Table 8.

TABLE 8 Example 8 in mm f = 7.05 Fno = 2.01 ω(°) = 35.5 ih = 5.06 TTL =8.66 Surface Data Surface Curvature Surface Refractive Abbe No. i Radiusr Distance d Index Nd Number νd (Object Surface) Infinity Infinity 1(Stop) Infinity −0.589  2* 2.968 1.000 1.5438 55.57  3* 100.000 0.049 4* 3.187 0.280 1.6391 23.25  5* 2.113 0.807  6* −100.000 0.375 1.543855.57  7* 119.100 0.228  8* 7.612 0.888 1.5438 55.57  9* −104.117 0.29610* −2.842 0.612 1.6391 23.25 11* −3.793 0.206 12* 4.611 1.078 1.543855.57 13* 12.267 0.878 14* −67.257 0.950 1.5438 55.57 15* 4.145 0.220 16Infinity 0.210 1.5168 64.20 17 Infinity 0.655 (Image Plane) InfinityConstituent Lens Data Lens Start Surface Focal Length 1 2 5.60 (=f1) 2 4−10.92 (=f2) 3 6 −99.90 (=f3) 4 8 13.08 (=f4) 5 10 −23.68 (=f5) 6 1212.94 (=f6) 7 14 −7.15 (=f7) Lens Composite Focal Length 3rd Lens-5thLens 44.45 (=f.345) 6th Lens-7th Lens −28.24 (=f67) Aspheric SurfaceData 2nd Surface 3rd Surface 4th Surface 5th Surface 6th Surface 7thSurface 8th Surface k 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 A4 2.496E−03 4.159E−03 −4.087E−02  −5.062E−02 2.376E−05 −1.152E−02  −1.924E−02  A6 −3.122E−04  8.039E−04 1.221E−021.313E−02 −1.758E−03  3.042E−04 −6.454E−04  A8 1.430E−04 −2.641E−04 −2.252E−03  −2.530E−03  5.585E−04 4.443E−04 3.290E−04 A10 0.000E+001.007E−05 1.153E−04 1.515E−04 −2.178E−05  0.000E+00 0.000E+00 A120.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00A14 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 A16 0.000E+00 0.000E+00 0.000E+00 0.000E+00 0.000E+000.000E+00 0.000E+00 9th Surface 10th Surface 11th Surface 12th Surface13th Surface 14th Surface 15th Surface k 0.000E+00 0.000E+00 −7.226E−01 0.000E+00 0.000E+00 0.000E+00 −4.489E+00 A4 −1.775E−02  1.380E−021.555E−03 −1.257E−02  8.601E−03 −2.701E−02  −2.291E−02 A6 5.957E−043.493E−03 2.550E−03 8.640E−04 −4.926E−03  1.101E−03  2.499E−03 A8−1.140E−04  −8.567E−04  −5.015E−04  −1.058E−03  9.028E−04 3.866E−04−2.222E−04 A10 0.000E+00 7.675E−05 4.026E−05 2.893E−04 −1.127E−04 −5.222E−05   1.387E−05 A12 0.000E+00 0.000E+00 0.000E+00 −4.093E−05 8.856E−06 2.677E−06 −4.794E−07 A14 0.000E+00 0.000E+00 0.000E+002.179E−06 −3.819E−07  −5.824E−08   6.643E−09 A16 0.000E+00 0.000E+000.000E+00 0.000E+00 6.893E−09 3.689E−10  0.000E+00

In the imaging lens in Example 8, the fifth lens L5 has negativerefractive power and the sixth lens L6 has positive refractive power. Asshown in Table 9, the imaging lens satisfies a conditional expression(1), conditional expressions (4) to (8), conditional expressions (11) to(14), and conditional expressions (17), (18), (20), and (21).

FIG. 16 shows spherical aberration (mm), astigmatism (mm), anddistortion (%) of the imaging lens in Example 8. As shown in FIG. 16,each aberration is corrected properly.

Table 9 shows data on Examples 1 to 8 relating to the conditionalexpressions (1) to (21).

TABLE 9 Example 1 Example 2 Example 3 Example 4 Example 5 Example 6Example 7 Example 8 Conditional Expression −0.55 −0.55 −0.55 −0.63 −0.57−0.54 −0.31 −0.51 (1) −1.0 < f1/f2 < −0.15 Conditional Expression (2) 0.93  1.01  1.14  1.09  1.14  0.92 — — 0.5 < f5/f < 1.5 ConditionalExpression −3.00 −3.54 −4.99 −5.07 −4.03 −2.98 — — (3) −8.0 < f6/f <−1.0 Conditional Expression — — — — — — −17.70  −3.36 (4) −20 < f5/f <−1.0 Conditional Expression (5) — — — — — —  1.77  1.84 1.0 < f6/f < 3.0Conditional Expression (6) 32.32 32.32 31.60 32.32 32.32 32.32 32.3232.32 20 < νd1 − νd2 < 40 Conditional Expression (7) 55.66 55.66 55.6655.66 55.66 55.66 55.66 55.57 40 < νd3 < 75 Conditional Expression (8)55.66 55.66 55.66 55.66 55.66 55.66 55.66 55.57 40 < νd7 < 75Conditional Expression (9) 55.66 55.66 55.66 55.66 55.66 55.66 — — 40 <νd4 < 75 Conditional Expression (10) 30.09 30.09 29.99 29.99 29.99 30.09— — 20 < | νd5 − νd6 | < 40 Conditional Expression (11) − — — — — —32.41 32.32 20 < | νd4 − νd5 | < 40 Conditional Expression (12) — — — —— — 55.66 55.57 40 < νd6 < 75 Conditional Expression (13)  1.28  1.24 1.23  1.24  1.24  1.25  1.28  1.23 1.0 < TTL/f < 1.35 ConditionalExpression (14)  0.84  0.89  0.86  0.86  0.86  0.87  0.89  0.86 TTL/2ih< 1.0 Conditional Expression (15)  0.78  0.84  0.88  0.83  0.87  0.85 —— 0.4 < f345/f < 1.2 Conditional Expression −0.59 −0.60 −0.67 −0.64−0.65 −0.60 — — (16) −1.0 < f67/f < −0.3 Conditional Expression (17) — —— — — —  4.11  6.30 2.0 < f345/f < 8.0 Conditional Expression — — — — —— −3.16 −4.00 (18) −6.0 < f67/f < −2.0 Conditional Expression (19)  1.61 1.63  2.10  1.92  2.02  0.97 — — 0.8 < (r9 + r10)/(r9 − r10) < 2.5Conditional Expression — — — — — — −17.23 −6.98 (20) −20.0 < (r9 +r10)/(r9 − r10) < −4.0 Conditional Expression (21)  1.64  1.78  1.73 2.08  2.08  2.01  1.83  2.01 f/EPD < 2.40

As explained so far, the imaging lenses in the examples according tothis embodiment of the present invention are low-profile enough to meetthe growing demand for low-profileness, with a ratio of total tracklength to diagonal length (TTL/2ih) of 0.9 or less, though they useseven constituent lenses. In addition, the imaging lenses offer a widerfield of view of 70 to 75 degrees and brightness with an F-value of 2.1or less, and correct various aberrations properly and can bemanufactured at low cost.

When any one of the imaging lenses composed of seven constituent lensesin the examples according to this embodiment of the present invention isused in the image pickup device mounted in an increasingly compact andlow-profile mobile terminal such as a smartphone, mobile phone, tabletor PDA (Personal Digital Assistant), a game console, an informationterminal such as a PC, or a highly functional product such as a homeappliance with a camera function, it contributes to the compactness ofthe image pickup device and provides high camera performance.

The effects of the present invention are as follows.

According to the present invention, there is provided a compact low-costimaging lens which meets the demand for low-profileness, offers highbrightness and a wide field of view and corrects various aberrationsproperly.

1-20. (canceled)
 21. An imaging lens configured to form an image of anobject on a solid-state image sensor, in which the lenses are arrangedin order from an object side to an image side of the imaging lens andare spaced from each other, the imaging lens comprising: a first lenswith a positive refractive power; a second lens with a negativerefractive power; a third lens with a positive or a negative refractivepower; a fourth lens with a positive or a negative refractive power; afifth lens with a positive refractive power having a concave surfacefacing the object side near an optical axis and a convex surface facingthe image side near the optical axis; a sixth lens with a positive or anegative refractive power; and a seventh lens with a negative refractivepower, the seventh lens being a double-sided aspheric lens having aconcave surface facing the object side near the optical axis and aconcave surface facing the image side near the optical axis, wherein thethird lens, the fourth lens, the fifth lens, and the sixth lens eachhave at least one aspheric surface, the seventh lens has a pole-changepoint spaced from an optical axis of the imaging lens on its asphericimage-side surface, and an expression (6) is satisfied:20<vd1−vd2<40, where   (6) vd1: abbe number of the first lens at d-ray,and vd2: abbe number of the second lens at d-ray.
 22. The imaging lensaccording to claim 1, wherein an expression (1) is satisfied:−1.0<f1/f2<−0.15, where f1: a focal length of the first lens, and f2: afocal length of the second lens.
 23. The imaging lens according to claim1, wherein an expression (7) is satisfied:40<vd3<75, where   (7) vd3: abbe number of the third lens at d-ray. 24.The imaging lens according to claim 1, wherein an expression (8) issatisfied:40<vd7<75, where   (8) vd7: abbe number of the seventh lens at d-ray.25. The imaging lens according to claim 1, wherein an expression (9) issatisfied:40<vd4<75, where   (9) vd4: abbe number of the fourth lens at d-ray. 26.The imaging lens according to claim 1, wherein an expression (10) issatisfied:20<|vd5−vd6|<40, where   (10) vd5: abbe number of the fifth lens atd-ray, and vd6: abbe number of the sixth lens at d-ray.
 27. The imaginglens according to claim 1, wherein an expression (13) is satisfied:1.0<TTL/f<1.35, where   (13) f: an overall focal length of the imaginglens, and TTL: a distance along the optical axis from an image plane ofthe imaging lens to an object-side surface of an optical element locatednearest an imaged object.
 28. The imaging lens according to claim 1,wherein an expression (14) is satisfied:TTL/2ih<1.0, where   (14) TTL: a distance along the optical axis from animage plane of the imaging lens to an object-side surface of an opticalelement located nearest an imaged object, and ih: a maximum imageheight.
 29. The imaging lens according to claim 1, wherein an expression(19) is satisfied:0.8<(r9+r10)/(r9410)<2.5, where   (19) r9: curvature radius of theobject-side surface of the fifth lens, and r10: curvature radius of theimage-side surface of the fifth lens.
 30. The imaging lens according toclaim 1, wherein an expression (21) is satisfied:f/EPD<2.40, where   (21) f: an overall focal length of the imaging lens,and EPD: entrance pupil diameter.
 31. The imaging lens according toclaim 1, wherein an expression (2) is satisfied:0.5<f5/f<1.5, where   (2) f: an overall focal length of the imaginglens, and f5: a focal length of the fifth lens.